EP3673220A1 - Système de stockage d'énergie thermique à cycle fermé utilisant un matériau thermochimique - Google Patents

Système de stockage d'énergie thermique à cycle fermé utilisant un matériau thermochimique

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Publication number
EP3673220A1
EP3673220A1 EP18759090.6A EP18759090A EP3673220A1 EP 3673220 A1 EP3673220 A1 EP 3673220A1 EP 18759090 A EP18759090 A EP 18759090A EP 3673220 A1 EP3673220 A1 EP 3673220A1
Authority
EP
European Patent Office
Prior art keywords
pressure
air
reactor
water mixture
energy storage
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
EP18759090.6A
Other languages
German (de)
English (en)
Other versions
EP3673220B8 (fr
EP3673220B1 (fr
Inventor
Jelle HOUBEN
Petrus Adrianus Joseph DONKERS
Hendrik Pieter HUININK
Sebastiaan Joannes Franciscus ERICH
Olaf Clemens Gerardus ADAN
Mohammed Zuhair SIDDIQUI
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nederlandse Organisatie voor Toegepast Natuurwetenschappelijk Onderzoek TNO
Eindhoven Technical University
Original Assignee
Nederlandse Organisatie voor Toegepast Natuurwetenschappelijk Onderzoek TNO
Eindhoven Technical University
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Publication of EP3673220A1 publication Critical patent/EP3673220A1/fr
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Publication of EP3673220B1 publication Critical patent/EP3673220B1/fr
Publication of EP3673220B8 publication Critical patent/EP3673220B8/fr
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Classifications

    • F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F28—HEAT EXCHANGE IN GENERAL
    • F28D—HEAT-EXCHANGE APPARATUS, NOT PROVIDED FOR IN ANOTHER SUBCLASS, IN WHICH THE HEAT-EXCHANGE MEDIA DO NOT COME INTO DIRECT CONTACT
    • F28D20/00—Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00
    • F28D20/003—Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00 using thermochemical reactions
    • F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F28—HEAT EXCHANGE IN GENERAL
    • F28D—HEAT-EXCHANGE APPARATUS, NOT PROVIDED FOR IN ANOTHER SUBCLASS, IN WHICH THE HEAT-EXCHANGE MEDIA DO NOT COME INTO DIRECT CONTACT
    • F28D20/00—Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00
    • F28D20/0056—Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00 using solid heat storage material
    • F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F28—HEAT EXCHANGE IN GENERAL
    • F28D—HEAT-EXCHANGE APPARATUS, NOT PROVIDED FOR IN ANOTHER SUBCLASS, IN WHICH THE HEAT-EXCHANGE MEDIA DO NOT COME INTO DIRECT CONTACT
    • F28D20/00—Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00
    • F28D2020/0065—Details, e.g. particular heat storage tanks, auxiliary members within tanks
    • F28D2020/0078—Heat exchanger arrangements
    • Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E60/00—Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation
    • Y02E60/14—Thermal energy storage

Definitions

  • the present invention relates generally to thermal energy storage systems. More specifically, it relates to thermal energy storage systems using thermochemical materials.
  • thermochemical materials TCMs
  • TCM-based heat storage has several advantages compared to techniques like sensible heat storage and techniques using phase change materials. These advantages include nearly loss- free storage period and high energy density.
  • a gas-solid equilibrium reaction for a salt/salt-hydrate TCM can be represented by: wherein A -B is a solid salt complex made by combining a salt A(s) and reactive gas B(g).
  • reactive gas B is considered to be H 2 O, NH 3 or CH 3 OH.
  • the amount of reactive gas B inside salt complex A -B is called the loading of the salt.
  • the formation reaction of the salt complex A -B is exothermic, i.e., it produces energy that can be used for heating purposes.
  • the enthalpy of this formation reaction is ⁇ H ⁇ 0.
  • FIG. 1A shows a schematic illustrating such a TCM heat storage reaction.
  • the TCM 100 has two states, a salt complex 102 and a salt 104.
  • the TCM charging 106 involves the absorption of heat 108 by the TCM 100 and the release of water 110. The charging is thus also referred to as dehydration.
  • the TCM discharging 112 involves the release of heat 114 by the TCM 100 and the sorption of water 116. The discharging is thus also referred to as hydration.
  • Discharging and charging state diagrams are shown in FIG. IB and FIG. 1C, respectively.
  • the main criteria of success for such storage technique in for buildings are: high efficient energy density, cost efficiency (short payback time), safety, and durability.
  • TCMs For conventional heat storage based on TCMs, two main concepts are generally considered: 1) closed systems which store their own water and operate at vacuum pressures equal to the water vapor pressure at the condenser/evaporator (e.g., at 7.5 °C the pressure 10 mbar); and 2) open systems which exchange water with the environment and operate at constant atmospheric pressure.
  • a schematic drawing for both concepts is given in FIG. 2.
  • the TCM 200 in an open system 202 does not store its own water, but exchanges water with a water source 204 in the environment outside the system, which operates at constant atmospheric pressure.
  • a closed system 206 the water source 204 is included inside the system, which operates at vacuum pressure.
  • both compartments 200, 204 are part of the system and all water necessary for the hydration/dehydration reactions is stored within the system. Consequently, this means a large system size, and thus an effective decrease of the overall energy storage density.
  • the conventional closed system design has high demands on vacuum level ( ⁇ 10 mbar) and purity of the TCM. A small amount of non-condensable gasses will reduce the power or even stop the hydration or dehydration process in the reactor completely as a result of accumulation of non-condensable gasses at the condensation interface.
  • a traditional closed system is expensive and has a large environmental footprint as a result of the large amount of material in the heat exchanger in direct contact with the TCM.
  • TCM-based heat storage system designs have shortcomings that hamper the introduction of heat storage with TCMs, such as energy density, temperature output and system/material demands. There is thus a need for improved TCM-based heat storage systems.
  • the invention provides a new design for a thermal energy storage system using a thermochemical material (TCM).
  • TCM thermochemical material
  • it is a closed cycle system in which a TCM reactor containing a TCM is separated in the cycle from the heat exchanger.
  • the system operates with forced convection of air/water mixture at a controlled pressure that varies between a reduced pressure and an overpressure, tuned to produce desired temperature difference across the TCM reactor.
  • the system may be tuned or calibrated using measurements of water absorbed by the reactor.
  • the system does not require high vacuum (i.e., pressures below 10 mbar) and associated complexity of conventional closed systems. Operation with forced convection of gas and pressure control allows tuning of desired output temperature.
  • the TCM may be any solid TCM, such as salts (hydrates/ammoniates/methanol complexes), molecular sieves (zeolites), metal organic frameworks (MOFs), silicagel, or activated alumina.
  • the reduced pressure is a pressure below 1 atmosphere, while the overpressure is a pressure above one atmosphere.
  • the specific pressure will depend on the choice of particular TCM. For example, in one embodiment the reduced pressure is 200-400 mbar and the overpressure is 10 bar by an evaporator/condenser at 10 °C.
  • conventional TCM energy storage systems include only open systems (exchanging water with the environment and operating at atmospheric pressure) or traditional closed systems (storing their own water and operating at high vacuum).
  • Embodiments of the present invention do not operate at constant pressures of high vacuum or atmospheric pressure, but have active control of the system pressure in order to control the temperature difference across a TCM reactor. They may optionally be calibrated using measurements of partial pressure of H 2 O.
  • Embodiments have an adjustable pressure system with forced convection of the gas.
  • the temperature increase of the gas over the reactor bed can be actively controlled by changing the gas pressure in the reactor system.
  • the gas is blown actively through the reactor and presence of non-condensable gasses will not affect the performance of the system.
  • there are lower technical demands on the vacuum system as the pressure in the range of 10 mbar to 10 bar (absolute pressure) can be maintained by periodic and/or controlled pumping. Forced convection is used to avoid blocking of the evaporator/condenser or reactor bed by non-condensables.
  • the water is transported by an increased pressure of the carrier gas (i.e., pressure more than 1 bar).
  • This smaller temperature step will decrease heat losses within the system and the volume flow can be reduced.
  • the temperature step over the reactor can be controlled actively by varying the pressure of the reactor, based on the desired input and output temperature.
  • the system may be calibrated by measuring the water vapor content and temperature step at the output side of the bed.
  • the temperature increase/decrease of the gas over the reactor bed during hydration/dehydration can be actively controlled by changing the vapor pressure in the reactor system. Pressures in the range of 10 mbar to 10 bar (absolute pressure) can be maintained by periodic pumping.
  • Power output can be characterized by measuring the mass flow rate of gas, flow, or temperature increase of gas over reactor bed.
  • FIG. 1A is a schematic illustration of a TCM heat storage reaction using a salt TCM.
  • FIGS. IB and 1C are discharging and charging state diagrams, respectively, for a TCM heat storage reaction of FIG. 1A.
  • FIG. 2 is a schematic drawing illustrating the difference between conventional open and closed
  • FIGS. 3A and 3B are graphs of temperature and power, respectively, vs. the pressure in a TCM heat storage system, illustrating the effects of the evaporator temperature of the optimal hydration pressure.
  • FIG. 4 is a schematic overview of an illustrative embodiment of a hybrid design for a TCM heat storage system during production of heat.
  • FIG. 5 is a graph of temperature step across the TCM reactor bed vs water vapor pressure, illustrating the effect of reduced gas pressure on the temperature step.
  • FIGS. 6 A and 6B are a schematic diagrams of a semi-closed TCM heat storage system during charging and discharging, respectively.
  • FIGS. 7A and 7B are a schematic diagrams of a semi-open TCM heat storage system during charging and discharging, respectively.
  • a conventional closed system has high demands on its vacuum level and purity of the TCM. A small amount of non-condensable gasses will reduce the power or even stop the hydration or dehydration process in the reactor completely.
  • a closed system is an expensive technique and has a large environmental footprint as a result of the large amount of material in the heat exchanger.
  • the main advantages of a conventional closed reactor vacuum system is that the mass transport from the evaporator to the TCM is fast and has an inherent driving force (namely, the vapor pressure difference between evaporator and TCM). Thus, the reactor consumes no energy for the vapor transport during heat production. Secondly, the output temperature of the reactor is not limited by the reactor, but by the TCM and applied vapor pressure. The closed system also has the potential for cooling.
  • the conventional closed system has the disadvantage that the performance of the reactor decreases dramatically by a non-condensable gasses as these cause gas to accumulate at the condenser as a result of gas flow counterbalancing the driving force. This results in high demands on system (leakage) and material level (outgassing of non-condensable gasses).
  • the TCM in the closed system design is in direct contact with the heat exchanger.
  • the heat exchanger should be able to withstand long term exposure of wet salts, and it should be large to contact all the TCM. In general, the demands on the heat exchanger materials are high, which results in high investment costs.
  • Other disadvantages include: Output power is not easily adjusted, reduced energy density as water has to be stored in the reactor and heat exchanging material, maintenance costs are high as the heat exchanger is integrated with the TCM, and large amounts of heat exchanging material negatively affect the durability.
  • an open storage concept is less demanding on system level, cost effective, but cannot reach high output temperatures, as the heat capacity is too large for the gas delivering the vapor at low water vapor pressures (needed for the reaction to release the heat) to fully heat-up, causing low output temperatures.
  • the added heat is insufficient for a complete dehydration.
  • more air has to be blown through the reactor, which results in higher energy consumption during charging of the TCM system.
  • An open system also has adjustable output power by controlling the mass flow rate. In addition, part of the outside humidity can be used in the reactor, and water does not have to be stored.
  • a different gas flow rate cannot increase this value, as not enough water would be supplied, thus the temperature output is limited by the reactor design, not by the properties of the TCM.
  • Other disadvantages of an open system are energy consumption during heat production by devices used to force circulation of air through the system, and pressure drop over the bed requires significant energy.
  • current heat storage system designs have specific shortcomings that hamper the introduction of the heat storage with TCMs, such as energy density, temperature output and system/material demands.
  • a preferred embodiment of the system includes the following components arranged in a closed cycle: TCM reactor bed 400, heat exchanger 402, pressure adjustment pump 404, forced convection fan 406, evaporator/condenser 408, and conduits 414, 416, 418, 420 connecting the components into a closed cycle, as shown. It is noted that the reactor 400 and the heat exchanger 402 are distinct components separated by a conduit rather than being a single integrated component. This separation makes it possible to design the heat exchanger separately from the TCM.
  • the storage capacity (the amount of TCM in the reactor) is no longer related to the amount of heat exchanger material, what is the case in a closed system.
  • the fan is not needed.
  • the forced convection may be produced by a pressure difference across the reactor, with no fan needed.
  • the system also includes a sensor 422 for measuring a physical property of the gas, such as pressure or flow, from which the current pressure of the system may be determined directly or indirectly.
  • a controller 424 sends signals to the pump 404 to create a desired system pressure in order to achieve a desired temperature output.
  • the system may optionally include relative humidity sensors 410, 412 positioned on opposite sides of reactor bed 400 for purposes of calibrating the performance of the system.
  • the density of water and gas can be calculated according to the following equations with the assumption that we are dealing with ideal gasses:
  • the temperature lift in a closed-loop reactor may be controlled by adjusting the pressure of the heat transferring medium (HTM).
  • HTM heat transferring medium
  • ⁇ H reaction is the reaction energy of the reaction A+B->A B (J/mol)
  • M gas is the molar mass of the used gas (g/mol)
  • heat capacity of the used gas is the
  • the efficiency of the reactor with a constant dehydration temperature can be controlled by:
  • FIGS. 3A and 3B an example is given of the effects of the evaporator temperature of the optimal hydration pressure. As can be seen, by higher evaporator temperatures a higher pressure in the system will result in optimal performance. Too high pressures result in decreased output temperatures, too low pressures in lower power outputs.
  • the temperature and power in FIGS. 3A and 3B are plotted against the pressure in the system for three evaporator/condenser temperatures with an inlet temperature of 30 °C and limited output temperature of 59 °C. The temperature lift at lower pressures is limited by the material properties, which has negative effects on the power output at lower pressures.
  • the stars indicate the optimal conditions in case of temperature and power output for the different E/C temperatures.
  • Embodiments of the present invention combine features of the open and closed configurations to overcome their disadvantages.
  • a forced convection is used to avoid blocking of the evaporator/condenser or reactor bed by non-condensable gasses.
  • the water is transported by a reduced pressure of the carrier gas. This increases the temperature step over the reactor bed, as the same amount of energy is supplied, but less mass has to be heated up.
  • the temperature step over the reactor can be controlled actively by adjusting the pressure of the reactor, based on the desired input and output temperature. The relation between desired temperature step and corresponding pressure may be determined during design or calibration by measuring the water vapor content on both sides of the reactor bed.
  • a forced convection is used (0-30 g H 2 O /s, depending on the desired power output).
  • the pressure may be varied between 10 mbar and lO bar, preferably between 200-400 mbar during hydration and 1-2 bar during dehydration, strongly dependent on conditions like evaporator/condenser temperature (water vapor pressure) and dehydration temperatures.
  • the TCM in this example is K 2 CO 3 - 1.5H 2 O/ K 2 CO 3 .
  • the thermal energy storage system includes the following separate components arranged in a closed cycle: a thermochemical reactor 400 containing a solid thermochemical material, a heat exchanger 402, a fan 406, and an evaporator/condenser 408. These components are connected by gas conduits 414, 416, 418, 420. Fan 406 is understood herein to encompass any device suitable for creating a forced convection of gas, so as to induce the gas to circulate around the close cycle.
  • the system also includes an adjustable pressure control system for actively controlling the pressure of the air/water mixture to produce a desired temperature difference across the thermochemical reactor.
  • the pressure control system includes a vacuum pump 404, a gas property sensor 422 that senses a physical characteristic (such as pressure) of the air/water mixture, and a controller 424 that is configured to control the pressure of the air/water mixture by sending appropriate control signals to the pump 404, based in part on measurements from the gas property sensor 422.
  • the pressure of the air/water mixture is adjusted to an underpressure during a hydration phase and an overpressure during a dehydration phase.
  • the underpressure is selected to be a pressure above 10 mbar and below 1 bar, while the overpressure above is selected to be a pressure above 1 bar and below 10 bar.
  • the particular underpressure value and overpressure value are determined from a desired temperature drop.
  • the relationship between the desired temperature drop and the corresponding system overpressure and underpressure may be determined during system design and/or calibration using two relative humidity sensors 410, 412 positioned on opposite sides of the thermochemical reactor 400.
  • the relative humidity sensors 410, 412 are not necessary components of the system, as they are not needed once the system design has been fixed.
  • Operation of the closed cycle thermal energy storage system includes determining from the gas property sensor a pressure of an air/water mixture circulating in the system, and actively controlling the pressure of the air/water mixture to produce a desired temperature difference across the thermochemical reactor.
  • Gas e.g., air, N 2 , other carrier
  • This gas will pass evaporator/condenser 408 to control the vapor pressure at the inlet of the reactor bed 400.
  • the water will be absorbed by the TCM and heat will be released.
  • the produced heat will be transported with the gas to heat exchanger 402.
  • the pressure in the reactor can be adjusted at any time to a desired value with an extra inlet and outlet pump 404.
  • the pressure is selected to a value to achieve desired temperature and power output of the reactor.
  • the air will take up a certain amount of water which will be released by passing it through the evaporator/condenser unit.
  • the airflow is wetted by the evaporator/condenser.
  • the heat is transported by the air into the heat exchanger, where it will be harvested.
  • a reactor bed 400 A volume where the TCM is located and a volume flow can pass through for wetting and drying of the TCM. Pressure drop over the bed is preferably less than 1000 Pa (10 mbar), in order to drive the flow through the bed.
  • a heat exchanger 402 (air/air; air/liquid; air/(liquid/air)) is included to remove or add heat from/to the airflow inside the reactor to/from an external air or liquid flow.
  • the power range may be, for example, between 0.1-10 kW.
  • Fan 406 for forced convection through the reactor The volume flow of this fan strongly depends on the demanded power output of the reactor. I.e., for 1 kW the volume flow is in the order of 40 1/s by 100% efficiency.
  • the fan can create flow in forward and backward direction, as for charging the TCM the air should be heated before it enters the reactor bed and for discharging the air should be wetted before it enters the reactor bed. For example, 0-3000 m 3 /h for 0-4 kW application, preferably between 0 and 576 m 3 /h (40*3600*4 dm 3 /h) with 100% efficiency for 4 kW applications. 4.
  • An evaporator/condenser 408 is located between the air fan and reactor bed to control the water vapor pressure. During heat charging (dehydration) the partial water vapor pressure will be reduced at the condenser and during discharging the partial water vapor pressure will be increased.
  • Different types of evaporator/condensers can be used, for example dynamic (i.e. free falling film evaporator/condenser) and static (i.e. liquid water surface). Example power is 0.1-10 kW.
  • Vacuum pump/pressure pump 404 for controlling the overall pressure within the system.
  • the vacuum pump preferably is able to control the pressure inside the system between 10 mbar and 10 bar at roughly 0.2 bar/m 3 per hour.
  • the system may include two RH sensors 410, 412 to measure the humidity before and after the TCM reactor. This information is important during calibration and/or design to determine the temperature lift for a given pressure.
  • the sensors preferably are able to work between 20-120 °C.
  • a pressure sensor 422 measures the total pressure of the system for use by controller to control the vacuum pump to achieve appropriate pressure to produce desired temperature drop. Pressure sensors may also be included optionally on both sides of the TCM reactor for determining when maintenance is needed (as the pressure drop is above a certain level) and if the expected pressure drop is present (range 1 mbar - 10 bar).
  • FIG. 5 is a graph of the effect of reduced gas pressure in the closed cycle reactor on the ⁇ for different water vapor pressues and efficiency of water uptake in the reactor bed. Efficiency is calculated by In the figure the system uses air as gas and K 2 CO 3 as TCM.
  • FIG. 6A-B is a schematic overview of charging and discharging of a semi-closed system.
  • charging air circulates around counter-clockwise in a closed cycle from TCM 600 to evaporator/condenser 602 to fan 604 to heat exchanger 608 and back to TCM 600.
  • discharging FIG. 6B
  • the pressure within the system is controlled with a pump 606.
  • the pressure inside will in most cases be smaller than 1 bar.
  • the pressure inside will in most cases be increased above 1 bar.
  • the pressure inside the system will be tuned, such that the reactor will perform optimal and finally will reach a constant pressure.
  • Targeted leakage rate of the system is max 1 mbar a day.
  • Other features of this example system include:
  • Fan is preferably able to run in both directions (e.g., can be solved by tubing).
  • FIG. 7A-B is a schematic overview of charging and discharging of a semi-open heat storage system.
  • air is circulated in an open cycle from the inlet 706, to air/air heat exchanger 710 to a heat exchanger 714 and then through tubing 712 to the TCM 700.
  • TCM 700 the gas flows through tubing 702 back to the air/air heat exchanger 710 and the outlet 704, 708.
  • discharging FIG. 7B
  • the pressure within the system is controlled with a pump at the inlet 706. During discharging of the system, the pressure inside will in most cases be smaller than 1 bar.
  • the pressure inside will in most cases be increased above 1 bar.
  • the pressure inside the system will be tuned, such that the reactor will perform optimally, and finally will reach a constant pressure.
  • the forced convection in this embodiment will be a result of pressure drop in the system and the pump at the inlet.
  • the reactor functions as a device to induce forced convection.
  • the air In a semi open system, the air is refreshed with outside air. Therefore the incoming air will have a vapor content equal to the outside conditions.
  • the flow within the system can be controlled with a fan and the pressure within the system by varying the outflow and inflow conditions with a pump.
  • the pressure inside will in most cases be smaller than 1 bar.
  • the pressure inside will in most cases be increased above 1 bar.
  • the TCM has to heat up, which means that the efficiency of the reactor material is different.
  • the pressure inside the system will be tuned, such that the reactor will perform optimal and finally it will reach a constant pressure.
  • a vacuum/pressure pump is used, with high volume flow.
  • control algorithm can be used to characterize and calibrate a particular system to determine overpressure and underpressure values for desired temperature drops.
  • the drop in water content (AP H2O ) can be calculated.
  • step 1 till 5 is repeated indefinitely.
  • step 1 till 5 is an infinite loop.
  • the pressure can be controlled to reproducibly create a desired temperature drop, e.g., using an empirical formula relating desired temperature to pressure, or a lookup table.

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  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Thermal Sciences (AREA)
  • Mechanical Engineering (AREA)
  • General Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • General Chemical & Material Sciences (AREA)
  • Physical Or Chemical Processes And Apparatus (AREA)

Abstract

La présente invention concerne un système de stockage d'énergie thermique à cycle fermé qui comprend un réacteur thermochimique [400] contenant un matériau thermochimique solide, un échangeur de chaleur [402], un ventilateur [406] pour créer une convection forcée d'un mélange air/eau circulant autour du cycle fermé, un évaporateur/condenseur [408], et un système de commande de pression qui comprend un capteur de pression [422], un dispositif de commande [424] et une pompe [404]. Le système de commande de pression commande activement la pression du mélange air/eau pour produire une différence de température souhaitée à travers le réacteur thermochimique [400]. Le système de commande de pression réglable commande la pression du mélange air/eau à une première pression (par exemple, entre 10 mbar et 1 bar) pendant une phase d'hydratation et une seconde pression (par exemple, entre 1 bar et 10 bars) pendant une phase de déshydratation.
EP18759090.6A 2017-08-22 2018-08-21 Système de stockage d'énergie thermique à cycle fermé utilisant un matériau thermochimique Active EP3673220B8 (fr)

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US201762548530P 2017-08-22 2017-08-22
PCT/EP2018/072574 WO2019038292A1 (fr) 2017-08-22 2018-08-21 Système de stockage d'énergie thermique à cycle fermé utilisant un matériau thermochimique

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EP3673220B1 EP3673220B1 (fr) 2023-06-28
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DK (1) DK3673220T3 (fr)
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FR2995062B1 (fr) 2012-09-04 2014-10-03 Commissariat Energie Atomique Procedes de stockage et de liberation d'energie thermique, reacteur associe et application au stockage intersaisonnier de chaleur solaire
US10386121B2 (en) 2013-10-21 2019-08-20 Advanced Cooling Technologies, Inc. Open-loop thermal management process and system
KR102543809B1 (ko) 2014-09-02 2023-06-16 네덜란제 오르가니자티에 포오르 토에게파스트-나투우르베텐샤펠리즈크 온데르조에크 테엔오 에너지의 열화학적 저장 시스템 및 방법
CN105423791A (zh) 2015-11-11 2016-03-23 上海交通大学 可调控化学蓄热系统
CN105651091B (zh) * 2016-02-19 2017-08-15 上海交通大学 传热增强型化学蓄热装置及应用该蓄热装置的蓄热系统

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WO2019038292A1 (fr) 2019-02-28
US11828540B2 (en) 2023-11-28
EP3673220B1 (fr) 2023-06-28
US20200355446A1 (en) 2020-11-12
DK3673220T3 (da) 2023-10-02
ES2960309T3 (es) 2024-03-04

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